[0001] The invention relates to a magnetic transducing head comprising a magnetic core having
two core limbs formed from a ferrite, which core limbs have two core faces facing
each other and at least one of which is provided with a cladding consisting of a layer
of an Fe-Si-Al-based alloy, a non-magnetizable transducing gap extending between the
core faces and a winding aperture with an electric coil passing therethrough and being
provided around a core limb.
[0002] A magnetic transducing head of this type is known and described,
inter alia in the publication IEEE 1984, September, Volume May 20, No. 5, pages 872-874, Analysis
Of Metal In Gap Heads, by J.J.M. Ruigrok.
[0003] The transducing heads which are used in present-day video recorders generally have
an Mn-Zn ferrite core. Mn-Zn ferrite has a saturation magnetization of approximately
0.5 Tesla at room temperature, which is sufficient to comply with the requirements
imposed by the registration on conventional video tapes, such as CrO₂-tapes with a
coercive force Hc of approximately 56 kA/m. If, however, magnetic tapes having a higher
coercive force such as Fe-tapes which have a Hc of rougly 80-160 kA/m are used for
improving the quality of the video registration, such magnetic tapes can no longer
be written satisfactorily. The magnetic fields generated by the transducing head at
the area of the transducing gap for writing information on the magnetic tape are in
fact limited by the relatively low saturation magnetization of the ferrite in the
transducing head core. The strength of the writing field of the transducing head is
therefore insufficiently high to ensure optimum writing of magnetic tapes with a high
coercive force.
[0004] In the known transducing head defined in the opening paragraph the above-described
problem is tackled by sputtering a layer of Fe-Si-Al on at least one of the core faces
present on either side of the transducing gap. In fact, the Fe-Si-Al alloy sputtered
on the core faces enhance the recording and reproducing characteristics of the transducing
head. In addition Fe-Si-Al is a wear-resistant material so that hollow-out of the
transducing head owing to moving a magnetic tape along the tape contact face of the
transducing head can be mitigated.
[0005] A drawback of the known transducing head is that pseudo-gaps or side gaps are formed
between the ferrite core limbs and the Fe-Si-Al layers so that constructive and destructive
interferences causing troublesome oscillations in the frequency characteristic of
the known transducing head may occur at the area of the interfaces between the core
limbs and the Fe-Si-Al layers.
[0006] To reduce the detrimental effect of the occurrence of pseudo-gaps in magnetic heads
with a ferrite core it has been proposed in the publication Digests of Intermag 85,
April 29-May 2, USA, p. DA-1, A tilted sendust-sputtered ferrite video head, by T.
Kobayashi, c.s. to position the faces in which the pseudo-gaps occur in such a way
that the psuedo-gaps do not run parallel to the transducing gap, but constitute an
angle with this gap.
[0007] A magnetic head in which this measure is used is indeed less subject to pseudo-gap
effects, but a magnetic head of this type is rather complicated in its construction
and difficult to manufacture from a technological point of view.
[0008] It is an object of the invention to improve the transducing head defined in the opening
paragraph in such a way that the problem of the occurring pseudo-gaps is solved in
a technologically simple manner.
[0009] To this end the transducing head according to the invention is characterized in that
the cladding provided on the core face also comprises a layer of an Ni-Fe-based alloy,
the layer of an Ni-Fe-based alloy being provided on the core face and the layer of
an Fe-Si-Al-based alloy being provided on the layer of an Ni-Fe-based alloy.
[0010] In the transducing head according to the invention no pseudo-gaps are produced at
the transition of the ferrite core limb to the layer of an Ni-Fe-based alloy, nor
at the transition of the layer of an Ni-Fe-based alloy to the layer of an Fe-Si-Al-based
alloy, which is also clearly evident from the favourable frequency characteristics
of the transducing head in which perterbations caused by possible side gaps are not
present.
[0011] The transducing head according to the invention can be manufactured in a simple manner
in accordance with known techniques in which the different layers are provided one
after the other, for example by means of sputtering.
[0012] A main embodiment of the transducing head according to the invention, which has very
good properties for writing information on high coercive registration media and which
can be manufactured in an economically attractive way is characterized in that the
said cladding is provided on both core faces, whilst parallel gap boundary faces of
equal width for defining the gapwidth of the transducing gap are formed, central core
face parts parallel to the gap boundary faces extending between the core limbs and
the claddings thereof, and oblique core face parts constituting an angle with the
central core face parts extending on either side thereof, the said central core face
parts having a width which is larger than half the width of the gap boundary faces.
[0013] In the transducing head according to the invention the cladding may be considerably
thinner than in the known magnetic heads as described, for example in European Patent
Application 0,125,891. This has the advantage that the cladding can be provided without
any complications on the core faces in accordance with known methods such as sputtering.
[0014] An embodiment which is favourable from a manufacturing-technical point of view is
characterized in that the width of the central core face parts is at least substantially
equal to the width of the gap boundary faces.
[0015] A further favourable embodiment is characterized in that on either side of the transducing
gap between the core limbs and the claddings thereof there extend further core face
parts contiguous to the oblique core faces and running parallel to the central core
faces. This embodiment, which can be manufactured in a simple manner, is particularly
interesting because after sputtering the transducing head does not need to be provided
with recesses on either side of the transducing gap for the purpose of locally constricting
the tape contact face.
[0016] Particularly favourable results can be achieved when the above-mentioned embodiments
are also characterized in that the thickness of the cladding is defined by the relation:

,
in which
D₁ is the sum of the thicknesses of the layer of an Fe-Si-Al-based alloy and the layer
of an Ni-Fe-based alloy, W₁ is the gapwidth, M
b is the weighted saturation magnetization of the materials of the said layers and
M
f is the saturation magnetization of the ferrite. The weighted saturation magnetization
is herein understood to mean:
in which
t
s is the thickness of the layer of an Fe-Si-Al-based alloy, M
s is the saturation magnetization of this layer, t
p is the thickness of the layer of an Ni-Fe-based alloy and M
p is the saturation magnetization of this layer.
[0017] An alternative main embodiment of the transducing head according to the invention
is characterized in that the cladding is provided on both core faces, whilst parallel
gap boundary faces of equal width for defining the gapwidth of the transducing gap
are formed, the core faces parallel to the gap boundary faces extending between the
core limbs and the claddings thereof, and the said core faces having a width which
is larger than the width of the gap boundary faces, whilst the claddings on either
side of the transducing gap have side faces which extend from the gap boundary faces
to the said core faces and which constitute an acute angle with the core faces.
[0018] A high efficiency and a frequency characteristic in which a side gap effect is hardly
noticeable can be achieved with this transducing head according to the invention.
The particularly satisfactory measuring results are all the more surprising because
the constructive measures used in the transducing head are completely in contrast
with the prior art trend as described in the said EP 0,125,891.
[0019] In EP 0,125,891 a magnetic head is described whose core is coated on at least one
side of the transducing gap with a thick cladding of a magnetic material having a
higher saturation magnetization than the ferrite of the core. The cladding is at least
substantially provided on two core faces obliquely positioned with respect to the
gap boundary face formed by the cladding, which core faces are mutually positioned
in such a way that a core face parallel to the gap boundary face is formed between
the oblique core faces, which core face has a width which is at most equal to half
the width of the transducing gap but which is preferably minimal. In fact, it is asserted
in the said European Patent Application that with an increasing width of the central
core face there is such a side gap effect (contour effect) at the area of the transition
between the core and the cladding that the frequency characteristic of the magnetic
head is increasingly disturbed, whereas the side gap effect is hardly disturbing in
the case of the smallest possible width of the core face or in the case of a total
absence of the core face. However, the side gaps in the known magnetic head still
yield magnetic potential losses and consequently signal losses.
[0020] The magnetic head described in EP 0,125,891 has thick claddings of the order corresponding
to half the gapwidth of the magnetic head or half the trackwidth of the magnetic tape.
Thick claddings have the drawback that they are difficult to provide and therefore
require a complicated manufacturing technique. Moreover, a very narrow central core
face located between the oblique core faces is difficult to realise with the conventional
sawing techniques.
[0021] An additional advantage of the alternative main embodiment of the transducing head
according to the invention is the absence of oblique core faces. In fact, the faces
on which the claddings are provided need not be profiled, which simplifies the manufacture
of the magnetic heads quite considerably. The side faces of the claddings can be formed
by means of a laser technique known
per se during which treatment the gap is also provided at the desired width.
[0022] The angle constituted by the said side faces with the core faces will preferably
be approximately 45°, but good results have also been achieved with angles of between
20° and 70°.
[0023] The transducing head defined hereinbefore as an alternative main embodiment is preferably
also characterized in that the thickness of the cladding is defined by the relation:

which
D₂ is the sum of the thicknesses of the layer of an Fe-Si-Al-based alloy and the layer
of an Ni-Fe-based alloy, W₂ is the gapwidth, M
b is the weighted saturation magnetization of the materials of the said layers, M
f is the saturation magnetization of the ferrite and α is the angle between a side
face and a core face.
[0024] It is to be noted that the thickness of the layer of an Ni-Fe-based alloy is preferably
small with respect to the layer of an Fe-Si-Al-based alloy and does not essentially
contribute to the thickness of the total cladding. Furthermore it is to be noted that
for achieving the envisaged object it is unimportant that the material of one of the
two layers of the cladding has a higher permeability than the material of the other
layer.
[0025] The invention will now be described in greater detail, by way of example, with reference
to the accompanying drawings in which
Figure 1 is a diagrammatic perspective elevational view of a first embodiment of
the magnetic transducing head according to the invention,
Figure 2 is a similar elevational view of a second embodiment,
Figure 2A shows the frequency characteristic of the second embodiment,
Figure 3 is a plan view on a larger scale of part of the second embodiment,
Figure 4 is a plan view on a larger scale of part of a transducing head in accordance
with the second embodiment,
Figure 5 is an elevational view of a third embodiment of the transducing head according
to the invention, and
Figure 6 is a plan view on a larger scale of part of the third embodiment.
[0026] The magnetic transducing heads shown in the Figures are suitable for writing and
reading magnetic tapes having high coercive forces.
[0027] The transducing head of Figure 1 has a magnetic core consisting of two core limbs
1 and 3 and accommodating a winding aperture 5. The winding aperture 5 accommodates
a portion of a coil 7 wound around one of the core limbs. The core limbs 1 and 3,
which are formed from a ferrite, for example mono-crystalline Mn-Zn ferrite are fixed
together by means of an adhesive layer 9 of a non-magnetic material such as glass
or quartz. The core limbs 1 and 3 are provided with contact faces 1A and 3A, respectively,
on which a magnetic tape (not shown) is moved in the direction of the arrow A during
operation of the transducing head. Near the contact faces 1A and 3A the layer 9 constitutes
a non-magnetic transducing gap 11 extending between the core limbs 1 and 3, which
gap has a length of, for example approximately 0.3 µm.
[0028] In the embodiments shown the core limbs 1 and 3 each have a completely flat core
face 1B and 3B, respectively, facing the gap 11 on which faces a cladding consisting
of two layers 13 and 15 is provided. The core faces 1B and 3B on either side of the
transducing head are bounded by two recesses 17 which partly extend in the tape contact
face constituted by the contact faces 1A and 3A and partly extend as far as the side
faces of the transducing head. The layer 13 consists of an Ni-Fe-based alloy, such
as Ni₈₀Fe₂₀, and is provided on the core faces 1B and 3B by means of, for example
sputtering or vapour-deposition, whilst the layer 15 consists of an Fi-Si-Al-based
alloy such as FE
85.8Si
9.2Al
5.0 and is provided on the said layer 13 by means of sputtering, vapour-deposition or
another process.
[0029] If the Ni-Fe-based alloy is provided by means of sputtering, a mixture of Ar-N₂ gas
may be used during sputtering to increase the hardness of the sputtered alloy. The
use of such a gas during sputtering is known
per se and has been described,
inter alia, in DE 3342533.
[0030] It has been found by experiment that favourable results can be achieved with layer
thicknesses whose values are between 0.05 and 2.0 µm for layer 13 and between 1 and
10 µm for layer 15. These values are only examples because satisfactory results can
also be achieved beyond the limits indicated.
[0031] In the embodiment shown the transducing gap, viewed widthwise, is at right angles
to the direction of movement of the magnetic tape. Embodiments in which the transducing
gap in the direction viewed is not oriented at right angles to the said direction
of movement are of course also possible.
[0032] The transducing head 201 shown in Figure 2 is suitable for writing and reading magnetic
tapes having a high coercive force. The transducing head 201 has a magnetic core consisting
of two core limbs 203 and 205, which core is provided with a winding aperture 207
through which a coil 209 is wound. The core limbs 203 and 205, which consist of a
mono-crystalline Mn-Zn ferrite, are sealed together by means of a sealing material,
such as glass in the regions 211 and 213. In region 211 a transducing gap 215 is thus
formed. The core limbs 203 and 205 have a tape contact face 217 along which a magnetic
tape (not shown) is moved in the direction of the arrow A1 during operation of the
transducing head 201.
[0033] The visible parts of the transducing heads shown in Figures 3 and 4 have the same
reference numerals as the parts of the transducing head according to Figure 2 corresponding
to the said parts.
[0034] As is shown in Figures 2, 3 and 4, claddings are provided on the core limbs 203 and
205. The cladding consists of a layer 223 of an Ni-Fe-based alloy and a layer 225
of an Fe-Si-Al-based alloy. The claddings constitute two parallel gap boundary faces
225A and 225B, respectively (see particularly Figures 3 and 4) of equal width. These
gap boundary faces 225A and 225B define the gapwidth W1 of the transducing gap 215
which is filled with a non-magnetic material such as glass or quartz. The direction
in which the gapwidth is defined is oriented, at least in these embodiments, at right
angles to the direction of movement of the magnetic tape. Embodiments in which the
said two directions are not at right angles to each other or of course also possible.
[0035] According to the invention central core face parts 203A and 205A are present between
the core limbs 203 and 205 on the one hand and the claddings on the other hand, and
on either side of these core faces and contiguous thereto there are provided oblique
core face parts 203B and 205B constituting an angle with the central core face parts.
The central core face parts 203A and 205A are almost equal to the width of the gap
boundary faces. In the embodiments shown in Figures 2, 3 and 4 further core face parts
203C and 205C contiguous to the oblique core faces parts are provided, which extend
parallel to the central core face parts 203A and 205A. For the supply of flux to the
gap 215 at the tape contact face 217 it is favourable to cover not only the core face
parts 203A, B, C and 205A, B, C at the area of the transducing gap with a layer of
a magnetic material of the type described, but also the other face parts of the magnetic
core adjacent the said core face parts and facing the transducing gap 215, so that
the core limbs 203 and 205 are provided with a cladding on their sides facing the
gap 215 over the entire height
h. The claddings 223 and 225 may be provided during the manufacture of the transducing
heads on the core limbs 203 and 205 by means of, for example sputtering, electro-deposition
or vapour-deposition after the said core faces have been formed by means of, for example
sawing. After the claddings 223 and 225 are provided, the core limbs 203 and 205 can
be sealed together.
[0036] The magnetic head shown in Figure 4 has undergone an extra processing treatment in
which for the purpose of constriction of the tape contact face 217 in the neighbourhood
of the transducing gap 215 two recesses 219 have been provided by means of, for example
a laser.
[0037] For determining the thickness D1 of the cladding use can be made of the relation
already given in the introduction to the description. In the embodiment according
to Figure 1 the thickness D1 is 3 µm. The gapwidth W1 is preferably smaller than 18
µm.
[0038] Figure 2A shows the frequency characteristic with the output signal V as a function
of the measuring frequency
f of a transducing head of the type according to Figure 2 whose cladding consists of
a layer of an Ni-Fe-based alloy having a thickness of 0.5 µm and a layer of an Fe-Si-Al-based
alloy having a thickness of 2.5 µm. It can clearly be seen that oscillations hardly
occur in the frequency characteristic.
[0039] The tranducing head 101 according to the invention shown in Figures 5 and 6 has principally
the same properties as the transducing heads already described. The transducing head
101 has two core limbs 103 and 105 of ferrite which together form a magnetic core
with a tape contact face 117 along which an information carrier can be moved in the
direction shown by arow A2 for magnetic co-operation with the transducing head 101.
An electric coil 109 passing through a winding aperture 107 is provided around the
core limb 105. The core limbs 103 and 105 which are connected together by means of
a sealing layer 113 of, for example, glass each have a core face 103A and 105A, respectively.
The core faces 103A and 105A face each other and run parallel to each other. A cladding
composed of a layer 123 and a layer 125 is provided on each of the two core faces
103A and 105A. The layers 123 and 125 consist of an Ni-Fe-based alloy and an Fe-Si-Al-based
alloy, respectively. The claddings 125 constitute a gap boundary face 125A and 125B,
respectively of a predetermined width, with the direction in which the width is defined
being at right angles to the direction denoted by the arrow A2 in this embodiment.
The overall gap boundary faces bound a transducing gap 115 having a gapwidth W2. The
transducing gap is formed by means of a layer of a non-magnetizable material such
as quartz, which may also serve to seal the claddings 125 together.
[0040] In front of and behind the transducing gap 115 the two core limbs 103 and 105, respectively,
are wedge-shaped, as viewed in the direction of the arrow A2, it being essential according
to the invention that this wedge is also present in the claddings. This means that
the claddings 123 and 125 have side faces 123B1 and 125B1, respectively, which constitute
acute angles α with the core faces 103A and 105A, respectively. The side faces 123B1
and 125B1 of the claddings 123 and 125 as well as the further wedge shape of the core
limbs may be realized, for example by means of known laser techniques. In this example
angle α is equal to 45°. The sum, D2, of the thicknesses of the claddings 123 and
125 can be determined by means of the relation already mentioned in the introduction
to the description.
[0041] In the latter embodiment in which the gapwidth W2 is 20 µm and the said angle α is
45°, 5 µm is a favourable value for the thickness D2.
1. A magnetic transducing head comprising
- a magnetic core having two core limbs (1, 3; 203, 205; 103, 105) formed from a ferrite,
which core limbs have two core faces (1B, 3B; 203 A,B,C, 205 A,B,C; 103 A, 105A) facing
each other and at least one of which is provided with a cladding consisting of a layer
of an Fe-Si-Al-based alloy (15; 225; 125),
- a non-magnetizable transducing gap (11; 215; 115) extending between the core faces
and
- a winding aperture (5; 207; 107) with an electric coil (7; 209; 109) passing therethrough
and being provided around a core limb,
characterized in that
the cladding provided on the core face also comprises of a layer of an Ni-Fe-based
alloy (13; 223; 123), the layer of an Ni-Fe-based alloy being provided on the core
face and the layer of an Fe-Si-Al-based alloy being provided on the layer of an Ni-Fe-based
alloy.
2. A magnetic transducing head as claimed in Claim 1, characterized in that the said
cladding is provided on both core faces, whilst parallel gap boundary faces (225A,
225B) of equal width for defining the gapwidth of the transducing head are formed,
central core face parts (203A, 205A) parallel to the gap boundary faces extending
between the core limbs (203, 205) and the claddings thereof, and oblique core face
parts (203B, 205B) constituting and angle with the central core face parts extending
on either side thereof, the said central core face parts having a width which is larger
than half the width of the gap boundary faces.
3. A magnetic head as claimed in Claim 2, characterized in that the width of the central
core face parts (203A, 205A) is at least substantially equal to the width of the gap
boundary faces (225A, 225B).
4. A magnetic head as claimed in Claim 2 or 3, characterized in that further core face
parts (203C, 205C) extend on either side of the transducing gap (215) between the
core limbs (203, 205) and the claddings thereof, which core face parts are contiguous
to the oblique core face parts (203B, 205B) and are parallel to the central core faces
(203A, 205A).
5. A magnetic head as claimed in Claim 2, 3 or 4, characterized in that the thickness
of the cladding is defined by the relation:
in which
D₁ is the sum of the thicknesses of the layer of an Fe-Si-Al-based alloy and the layer
of an Ni-Fe-based alloy, W₁ is the gapwidth, M
b is the weighted saturation magnetization of the ferrite.
6. A magnetic transducing head as claimed in Claim 1, characterized in that the cladding
is provided on both core faces (103A, 105A), whilst parallel gap boundary faces (125A,
125B) of equal width for defining the gapwidth of the transducing gap (115) are formed,
the core faces parallel to the gap boundary faces extending between the core limbs
(103, 105) and the claddings thereof, and the said core faces having a width which
is larger than the width of the gap boundary faces, whilst the claddings on either
side of the transducing gap have side faces (123B₁, 125B₁) which extend from the gap
boundary faces to the said core faces and which constitute an acute angle with the
core faces.
7. A magnetic head as claimed in Claim 6, characterized in that the said angle has a
value of between 20° and 70°.
8. A magnetic head as claimed in Claim 6 or 7, characterized in that the thickness of
the cladding is defined by the relation:
in which
D₂ is the sum of the thicknesses of the layer of an Fe-Si-Al-based alloy and the layer
of an Ni-Fe-based alloy, W₂ is the gapwidth, M
b is the weighted saturation magnetization of the materials of the said layers, M
f is the saturation magnetization of the ferrite and α is the angle between a side
face and a core face.
1. Tête magnétique comportant
- un noyau magnétique ayant deux branches de noyau (1, 3; 203, 205; 103, 105) formées
d'une ferrite, branches de noyau qui ont deux faces de noyau (1B, 3B; 203 A,B,C, 205
A,B,C; 103A, 105A) opposées dont au moins une est prévue d'un revêtement se composant
d'une couche d'un alliage à base de Fe-Si-Al (15; 225; 125),
- un entrefer de transmission non magnétisable (11; 215; 115) s'étendant entre les
faces de noyau et
- un espace d'enroulement (5; 207; 107) traversé par une bobine électrique (7; 209;
109) prévue autour d'une branche de noyau,
caractérisée en ce que
le revêtement prévu sur la face de noyau comporte en outre une couche d'un alliage
à base de Ni-Fe (13; 223; 123), la couche d'un alliage à base de Ni-Fe étant prévue
sur la face de noyau et la couche d'un alliage à base de Fe-Si-Al étant prévue sur
la couche d'un alliage à base de Ni-Fe.
2. Tête magnétique conforme à la revendication 1, caractérisée en ce que ledit revêtement
est prévu sur les deux faces de noyau, et en ce que sont formées des faces de limitation
d'entrefer parallèles (225A, 225B) de largeur égale pour définir la largeur de l'entrefer
de la tête magnétique, des parties de face de noyau centrales (203A, 205A) parallèles
aux faces de limitation d'entrefer s'étendant entre les branches de noyau (203, 205)
et leurs revêtements, et des parties de face de noyau obliques (203B, 205B) formant
un angle avec les parties de face de noyau centrales s'étendant des deux côtés de
celles-ci, lesdites parties de face de noyau centrales ayant une largeur supérieure
à la moitié de la largeur des faces de limitation d'entrefer.
3. Tête magnétique conforme à la revendication 2, caractérisée en ce que la largeur des
parties de face de noyau centrales (203A, 203B) est au moins sensiblement égale à
la largeur des faces de limitation d'entrefer (225A, 225B).
4. Tête magnétique conforme à la revendication 2 ou 3, caractérisée en ce que, des deux
côtés de l'entrefer de transmission (215), entre les branches de noyau (203, 205)
et leurs revêtements, s'étendent d'autres parties de face de noyau (203C, 205C) contiguës
aux parties de face de noyau obliques (203B, 205B) et parallèles aux faces de noyau
centrales (203A, 205A).
5. Tête magnétique conforme à la revendication 2, 3 ou 4, caractérisée en ce que l'épaisseur
du revêtement est définie par la relation:
où
D₁ est la somme de l'épaisseur de la couche d'un alliage à base de Fe-Si-Al et de
l'épaisseur de la couche d'un alliage à base de Ni-Fe, W₁ est la largeur de l'entrefer,
M
b est la magnétisation de saturation pondérée de la ferrite.
6. Tête magnétique conforme à la revendication 1, caractérisée en ce que le revêtement
est prévu sur les deux faces de noyau (103A, 105A), et en ce que sont formées des
faces de limitation d'entrefer parallèles (125A, 125B), de largeur égale déterminant
la largeur de l'entrefer de transmission 115, les faces de noyau parallèles aux faces
de limitation d'entrefer s'étendant entre les branches de noyau (103, 105) et leurs
revêtements, lesdites faces de noyau ayant une largeur supérieure à la largeur des
faces de limitation d'entrefer, tandis que les revêtements prévus des deux côtés de
l'entrefer de transmission présentent des faces latérales (123B₁, 125B₁) s'étendant
à partir des faces de limitation d'entrefer jusqu'auxdites faces de noyau et formant
un angle aigu avec les faces de noyau.
7. Tête magnétique conforme à la revendication 6, caractérisée en ce que ledit angle
a une valeur se situant entre 20° et 70°.
8. Tête magnétique conforme à la revendication 6 ou 7, caractérisée en ce que l'épaisseur
du revêtement est définie par la relation:
où
D₂ est la somme de l'épaisseur de la couche d'un alliage à base de Fe-Si-Al et l'épaisseur
de la couche d'un alliage à base de Ni-Fe, W₂ est la largeur de l'entrefer, M
b est la magnétisation de saturation pondérée des matériaux desdites couches, M
f est la magnétisation de saturation de la ferrite et α est l'angle faite par une face
latérale et une face de noyau.
1. Magnetkopf mit:
- einem Magnetkern mit zwei aus einem Ferrit gebildeten Kernteilen (1, 3; 203, 205;
103, 105) mit zwei einander zugewandten Kernflächen (1B, 3B; 203 A,B,C, 205 A,B,C;
103 A, 105 A), von denen mindestens eine mit einer Verkleidung aus einer Schicht einer
Fe-Si-Al-Legierung (15; 225; 125) versehen ist,
- einem nicht-magnetisierbaren Übertragungsspalt (11; 215; 115), der sich zwischen
den Kernflächen erstreckt und
- einer Spulenkammer (5; 207; 107) mit einer hindurchgehenden und um einen Kernteil
vorgesehenen elektrischen Spule (7; 209; 109),
dadurch gekennzeichnet, daß
die auf der Kernfläche vorgesehene Verkleidung ebenfalls eine Schicht aus einer Ni-Fe-Legierung
(13; 223; 123) aufweist, wobei die Ni-Fe-Legierungsschicht auf der Kernfläche und
die Fe-Si-Al-Legierungsschicht auf der Ni-Fe-Legierungsschicht angebracht ist.
2. Magnetkopf nach Anspruch 1, dadurch gekennzeichnet, daß die genannte Verkleidung auf beiden Kernflächen vorgesehen ist, während parallele
Spaltbegrenzungsflächen (225A, 225B) gleicher Breite zum Definieren der Spaltbreite
des Magnetkopfes gebildet sind, wobei zentrale Kernflächenteile (203A, 205A) sich
parallel zu den Spaltbegrenzungsflächen erstrecken, und zwar zwischen den Kernteilen
(203, 205) und der Verkleidung derselben, und wobei schräge Kernflächenteile (203B,
205B) mit den sich auf beiden Seiten erstreckenden zentralen Kernflächenteilen einen
Winkel einschließen, wobei die zentralen Kernflächenteile eine Breite aufweisen, die
größer ist als die Hälfte der Breite der Spaltbegrenzungsflächen.
3. Magnetkopf nach Anspruch 2, dadurch gekennzeichnet, daß die Breite der zentralen Kernflächenteile (203A, 205A) der Breite der Spaltbegrenzungsflächen
(225A, 225B) mindenstens im wesentlichen entspricht.
4. Magnetkopf nach Anspruch 2 oder 3, dadurch gekennzeichnet, daß weitere Kernflächenteile (203C, 205C) sich auf beiden Seiten des Übertragungsspaltes
(215) zwischen den Kernteilen (203, 205) und der Verkleidung derselben erstrecken,
wobei diese Kernflächenteile an den schrägen Kernflächenteilen (203B, 205B) anliegen
und sich parallel zu den zentralen Kernflächen (203A, 205A) erstrecken.
5. Magnetkopf nach Anspruch 2, 3 oder 4,
dadurch gekennzeichnet, daß die Dicke der Verkleidung durch die nachfolgende Beziehung definiert ist:
in der D₁ die Summe der Dicken der Fe-Si-Al-Legierungsschicht und der Ni-Fe-Legierungsschicht
ist, W₁ die Spaltbreite ist und M
b die gewichtete Sättigungsmagnetisierung des Ferrits ist.
6. Magnetkopf nach Anspruch 1 , dadurch gekennzeichnet, daß die Verkleidung an beiden Kernflächen (103A, 105A) vorgesehen ist, während parallele
Spaltbegrenzungsflächen (125A, 125B) gleicher Breite zum Definieren der Spaltbreite
des Übertragungsspaltes (115) gebildet werden, wobei die Kernflächen sich parallel
zu den Spaltbegrenzungsflächen zwischen den Kernteilen (103, 105) und der Verkleidung
derselben erstrecken, und eine Breite haben, die größer ist als die der Spaltbegrenzungsflächen,
während die Verkleidung auf den beiden Seiten des Übertragungsspaltes Seitenflächen
(123B₁, 125B₁) aufweist, die sich von den Spaltbegrenzungsflächen bis an die Kernflächen
erstrecken und mit den Kernflächen einen scharfen Winkel einschließen.
7. Magnetkopf nach Anspruch 6, dadurch gekennzeichnet, daß der genannte Winkel einen Wert zwischen 20° und 70° aufweist.
8. Magnetkopf nach Anspruch 6 oder 7,
dadurch gekennzeichnet, daß die Dicke der Verkleidung durch die nachfolgende Beziehung definiert ist:
in der D₂ die Summe der Dicken der Fe-Si-Al-Legierungsschicht und der Ni-Fe-Legierungsschicht
ist, W₂ die Spaltbreite ist, M
b die gewichtete Sättigungsmagnetisierung der Materialien der genannten Schichten ist,
M
f die Sättigungsmagnetisierung des Ferrits und α der Winkel zwischen einer Seitenfläche
und einer Kernfläche ist.